Home |
Search |
Today's Posts |
|
#1
![]() |
|||
|
|||
![]()
On Feb 2, 4:47 am, (J. B. Wood) wrote:
In article .com, "K7ITM" wrote: On Jan 30, 11:13 pm, "camelot" wrote: Hi Tom, well, after few researches on several books, I found that the formula I provided by me works only for real Z0. The general formula valid in case Z0 is complex is the follow: S11=(Zin-Z0*)/(Zin+Z0) Hello, and I don't know where you obtained that formula but it's incorrect. S11 in terms of a reflection coefficient is given by your formula above but without the complex conjugate of Z0. I have seen reflection coefficients in technical journals defined with a complex conjugate Z0 as you have shown but that's not consistent with scattering or transmission line theory (unless Z0 is real). I know it seems counterintuitve but a source of complex Z0 would be matched (no voltage/current reflections) to a transmission line having the same characteristic impedance. This condition does not in general correspond to the condition of maximum power transfer from source to line. Conversely a line of complex Z0 impedance connected to a source of complex Z0* impedance represents maximum power transfer from source to line but we still have voltage and current "reflections" RELATIVE to Z0. What you have to keep in mind is that incident (forward) and reflected voltages/currents only have meaning when they are referenced to an impedance, say Z0. And to monitor steady-state incident and reflected waves you need to separate the steady-state voltage (or current) into these components using a bridge or directional coupler (sampling devices that are also designed to use Z0 (e.g. 50 + j0 ohms) as a reference). In most applications what I've said is moot since line impedance is usually real or very close to real and we are dealing with sources having real or very close to real impedances. Under these conditions the matched condition coincides with maximum power transfer. If you want an in-depth treatment of what I've attempted to summarize I recommend the chapter on circuit analysis in the "Electronic Designers' Handbook", ed. E.J. Giacoletto, published by McGraw-Hill. Sincerely, John Wood (Code 5550) e-mail: Naval Research Laboratory 4555 Overlook Avenue, SW Washington, DC 20375-5337 To amplify just a bit on what John wrote, it's convenient to express the S-parameters referenced to an impedance that's accepted by other people you want to exchange data with, so that they don't have to transform your data to match their reference. 50 ohms resistive is pretty universally accepted in the non-television RF industry. Bear in mind that the S parameters work just fine, even though the transmission lines you are working with may not be exactly 50 ohms resistive, or even close to 50 ohms. In such a case, of course, S11 will not have the same meaning as a reflection coefficient for that line. Part of the "universally accepted" aspect is that the vast majority of RF test equipment is built to take readings referenced to 50 ohms resistive. We take great care to make sure that things look as close to 50+j0 as practical, over a wide frequency range. That said, there are particular industries where other impedances are used. 75 ohms is used in the video and television industry more commonly than 50 ohms, and you can buy vector network analyzers whose native impedance is 75 ohms. We've also made equipment to match the "standard" reference impedances used by telephone services and the audio industry. Finally, to head off the nearly inevitable rant that (Z-Z0)/(Z+Z0), for a complex Z0, allows S11 to have a magnitude greater than unity for a passive load, yes, we know that's true, and it's really NOT a problem. Don't try to attach more physical significance to the reflection coefficient than is actually there. (John, I do rather wish you'd dropped the line at the beginning of your post that said I had written the short segment you quoted from my posting, since I didn't write any of it; it was only lines I'd quoted from the original by "camelot"...but I trust that will be fairly obvious to readers.) Cheers, Tom |
#2
![]() |
|||
|
|||
![]()
Hello,
I'd like to thank you for the specification you reported; it seems that my formula is not properly correct! All my doubts on that matter rose by a very particular problem I met during my work where s-parameter simulation of a particular circuit matches analytic calculations only using the "controversial" formula. If I'll find few minutes, just for curiosity, I'll post the details of problem ;-) Regards, Camelot |
#3
![]() |
|||
|
|||
![]()
On Feb 8, 11:00 pm, "camelot" wrote:
Hello, I'd like to thank you for the specification you reported; it seems that my formula is not properly correct! All my doubts on that matter rose by a very particular problem I met during my work where s-parameter simulation of a particular circuit matches analytic calculations only using the "controversial" formula. If I'll find few minutes, just for curiosity, I'll post the details of problem ;-) Regards, Camelot Yes, that will be interesting. I do hope you find time to post the problem in more detail. Cheers, Tom |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Amplifier output matching | Homebrew | |||
Is it possible to have a 1:1 SWR? | Antenna |